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《中国物理C》(英文)编辑部
2024年10月30日

LANDAU PARAMETER GIANT MONOPOLE AND QUADRUPOLE STATES IN THE RELATIVISTIC HARTREE APPROXIMATION

  • By using the Hartree approximation which includes vacuum fluctuation correction in a model relativistic quantum field theory,it is found that the relativistic Landau parameters and 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 mean-field theory.
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  • [1] J. D. Walecka, Ann. Phys. (N. Y.), 83(1974). 491.[2] B. D. Serot, J. D. Walecka, adv. Nucl. Phys.; 16, ed. J. W. Negele, E. Vogt (Plenum, N. Y,1986).[3] J. V. Noble, Nucl. Phys., A329(1979), 354.[4] T. Matsui, Nucl. phys., A370(1981), 365[5] S. Nishizaki, H. Kurasawa, T. Suzuki, Nucl. Phys., A462(1987), 687.[6] C. J. Horawitz, B. D. Serot, Nucl. Phys., A464(1987), 613.[7] S. A. Chin, Ann. phys. (N. Y.), 108(1977), 301.[8] M. Kohno, K. Ando, prog. Theor. Phys., 61(1979), 1065.[9] T. Suzuki, Prog. Theor. Fhys., 64(1980), 1627.[10] S. A. Chin, Phys. Lets., 62B(1976), 263.
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Get Citation
ZHU Chao-Yuan and QIU Xi-Jun. LANDAU PARAMETER GIANT MONOPOLE AND QUADRUPOLE STATES IN THE RELATIVISTIC HARTREE APPROXIMATION[J]. Chinese Physics C, 1990, 14(1): 76-84.
ZHU Chao-Yuan and QIU Xi-Jun. LANDAU PARAMETER GIANT MONOPOLE AND QUADRUPOLE STATES IN THE RELATIVISTIC HARTREE APPROXIMATION[J]. Chinese Physics C, 1990, 14(1): 76-84. shu
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Received: 1900-01-01
Revised: 1900-01-01
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LANDAU PARAMETER GIANT MONOPOLE AND QUADRUPOLE STATES IN THE RELATIVISTIC HARTREE APPROXIMATION

    Corresponding author: ZHU Chao-Yuan,
  • Shanghai Institute of Nuclear Physics,Academia Sinica

Abstract: By using the Hartree approximation which includes vacuum fluctuation correction in a model relativistic quantum field theory,it is found that the relativistic Landau parameters and 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 mean-field theory.

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