Quark Mean Field Model for Finite Nuclei and Hypernuclei

SHEN Hong

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《中国物理C》（英文）编辑部

2024年10月30日

Chinese Physics C> 2004, Vol. 28> Issue(12) : 1313-1316

Quark Mean Field Model for Finite Nuclei and Hypernuclei

SHEN Hong ^,

Department of Physics,Nankai University,Tianjin 300071,ChinaCenter of Theoretical Nuclear Physics,National Laboratory of Heavy Ion Accelerator of Lanzhou,Lanzhou 730000,China

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Abstract：
The quark mean field model, which describes the baryon using the constituent quark model, is applied to study the properties of finite nuclei and hypernuclei. The meson mean fields couple directly with the quarks and change the properties of baryons in nuclear medium. The quark mean field model provides satisfactory results on the properties of spherical nuclei and hypernuclei. it also predicts an increasing size of the nucleon as well as a reduction of the effective mass in the nuclear environment.

References

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SHEN Hong. Quark Mean Field Model for Finite Nuclei and Hypernuclei[J]. Chinese Physics C, 2004, 28(12): 1313-1316.

SHEN Hong. Quark Mean Field Model for Finite Nuclei and Hypernuclei[J]. Chinese Physics C, 2004, 28(12): 1313-1316. shu

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Received: 2003-11-29
Revised: 1900-01-01

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沈阳化工大学材料科学与工程学院沈阳 110142

Quark Mean Field Model for Finite Nuclei and Hypernuclei

SHEN Hong ^,

Corresponding author: SHEN Hong,

Department of Physics,Nankai University,Tianjin 300071,ChinaCenter of Theoretical Nuclear Physics,National Laboratory of Heavy Ion Accelerator of Lanzhou,Lanzhou 730000,China

Received Date: 2003-11-29
Accepted Date: 1900-01-01
Available Online: 2004-12-05

Abstract: The quark mean field model, which describes the baryon using the constituent quark model, is applied to study the properties of finite nuclei and hypernuclei. The meson mean fields couple directly with the quarks and change the properties of baryons in nuclear medium. The quark mean field model provides satisfactory results on the properties of spherical nuclei and hypernuclei. it also predicts an increasing size of the nucleon as well as a reduction of the effective mass in the nuclear environment.