One π-meson and One σ-meson Exchange Potentials at Finite Temperatures

Zheng Guotong; Su Rukeng

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2024年10月30日

Chinese Physics C> 1990, Vol. 14> Issue(S2) : 135-144

One π-meson and One σ-meson Exchange Potentials at Finite Temperatures

Zheng Guotong ,
Su Rukeng

Dcpanment of Physics, Hangzhou Teacher's College, Department of Physics, Fudan University, Shanghai

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Abstract：
On the basis of the field theory at finite temperature, the dependence of π-meson and σ-meson effective masses upon temperatures at nucleon level and one π and one σ exchange potentials are discussed. The dependence of the π and σ effective masses upon temperatures is found to be in good agreement with the results given by the Nambu-Jone-Lasinia model at quark level.

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[20]	Chen Tao , Su Rukeng . The One Pion Exchange Potential at Finite Temperature. Chinese Physics C, 1988, 12(S2): 131-136.

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Zheng Guotong and Su Rukeng. One π-meson and One σ-meson Exchange Potentials at Finite Temperatures[J]. Chinese Physics C, 1990, 14(S2): 135-144.

Zheng Guotong and Su Rukeng. One π-meson and One σ-meson Exchange Potentials at Finite Temperatures[J]. Chinese Physics C, 1990, 14(S2): 135-144. shu

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Received: 1989-06-22

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Supported by the National Natural Science Foundation of China and Science Foundation of State Commission of Education in China.

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沈阳化工大学材料科学与工程学院沈阳 110142

One π-meson and One σ-meson Exchange Potentials at Finite Temperatures

Zheng Guotong
Su Rukeng

Dcpanment of Physics, Hangzhou Teacher's College, Department of Physics, Fudan University, Shanghai

Received Date: 1989-06-22

Fund Project: Supported by the National Natural Science Foundation of China and Science Foundation of State Commission of Education in China.

Abstract: On the basis of the field theory at finite temperature, the dependence of π-meson and σ-meson effective masses upon temperatures at nucleon level and one π and one σ exchange potentials are discussed. The dependence of the π and σ effective masses upon temperatures is found to be in good agreement with the results given by the Nambu-Jone-Lasinia model at quark level.