One η-Meson Exchange Potential of Nucleon-Nucleon at Finite Temperature

  • By means of the imaginary-time Green's function method,the temperature dependences of the η-meson and nucleon interaction coupling constant and one one η-meson exchange potential are discussed.We find that when temperature increases to 215MeV,the coupling constant approaches to zero and the one η-meson exchange potential of nucleon-nucleon disappears.
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  • [1] R. Machleidt, K. Holinde and Ch Elster, Phys. Rep., 149(1987), 1.[2] R. K. Su and G. T. Zheng, Jour; of Phys,G16(1990), 203.[3] T. Chen and R. K. Su, Hing Energy Phys. and Nucl. Phys., 12(1988), 131.[4] 郑国桐,苏汝铿,高能物理与核物理,14(1990),325.[5] D.卢里,粒子和场,科学出版社,北京(1981),p.342.[6] A. L.费特,J. D.瓦立克,多粒子系统的量子理论,科学出版社,北京(1984),p.314.
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ZHENG Guo-Tong and SU Ru-Keng. One η-Meson Exchange Potential of Nucleon-Nucleon at Finite Temperature[J]. Chinese Physics C, 1992, 16(2): 131-136.
ZHENG Guo-Tong and SU Ru-Keng. One η-Meson Exchange Potential of Nucleon-Nucleon at Finite Temperature[J]. Chinese Physics C, 1992, 16(2): 131-136. shu
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Revised: 1900-01-01
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One η-Meson Exchange Potential of Nucleon-Nucleon at Finite Temperature

    Corresponding author: ZHENG Guo-Tong,
  • Department of Physics,Hangzhou Teacher's College,3100122 Department of Physics,Fudan University,Shanghai 200433

Abstract: By means of the imaginary-time Green's function method,the temperature dependences of the η-meson and nucleon interaction coupling constant and one one η-meson exchange potential are discussed.We find that when temperature increases to 215MeV,the coupling constant approaches to zero and the one η-meson exchange potential of nucleon-nucleon disappears.

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