Chiral Bag Model at Finite Temperature

HUANG Jing-Yi; CAI Sheng-Shan; HU Si-Zhu; SU Ru-Keng

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《中国物理C》（英文）编辑部

2024年10月30日

Chinese Physics C> 1992, Vol. 16> Issue(6) : 494-498

Chiral Bag Model at Finite Temperature

Department of Physics,Fudan University,Shanghai 200433

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Abstract：
By taking the thermodynamical contributions of the pion mesons cloud outside the bag into account,the chiral bag model is extended to finite temperature.The temperature dependence of the radius of the chiral bag and the critical temperature of quark deconfinement are given.

References

[1]

R. K. Su and Z, Hu, Phys. Lett., 141A(1989), 420[2] R. Goldflam and L. Wilets, Phys. Rev., 25C(1982), 1951.[3] F. Takagi, Phys. Rev., 35D(1987), 2226.[4] 毕品镇，郑挺方，苏汝铿，科学通报，31(1986),341.[5] R. Gagnon, Phys. Rev., 28D(1983), 2862.[6] R. K. Su and T. Chen, Jottr, of Phys., 20A(1987), 5939.[7] E. K. Wang, J. R. Li and L. S. Liu, Phys. Rev., 41D(1990), 2288.[8] S. Kagiyama, A. Nakamuta and A. Minaka, Prog. Theor, Phys., 75(1986), 319.[9] G. E. Brown and M. Rho, Phys. Lett., 82B(1979), 177. G. E. Brown, M. Rho and V. Vento, Phys. Lett:，97B(1980), 423. [10]苏汝铿，统计物理学，复旦大学出版社，1990,p. 240,[11]赖德，基本粒子和对称性，宋孝同等译，科学出版社,1983,p. 107[12]R. D. pisarski, Phys, Lett., 110B(1982), 155.

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[3]	Deng Shenghua , Wang Enke , Li Jiarong . Two-Loop Effective Potential of Non-topological Soliton Bag Model at Finite Temperature. Chinese Physics C, 1995, 19(8): 713-726.
[4]	Zheng Taiyu . Casimir Effect at Finite Temperature. Chinese Physics C, 1995, 19(3): 241-244.
[5]	Gao Shouen , Hut Yuan , Zheng Guotong , Su Rukeng . η-meson in the Pseudoscalar Coupling at Finite Temperature. Chinese Physics C, 1994, 18(2): 148-153.
[6]	QIAN Zhi-Xin , ZHONG Wan-Heng , SU Ru-Keng . Yukawa Potential at Finite Temperature and Finite Density. Chinese Physics C, 1993, 17(5): 417-422.
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[9]	DENG Sheng-Hua , LI Jia-Rong . Disappearance of Chiral Soliton Solutions and Chiral Phase Transition at High Temperature. Chinese Physics C, 1993, 17(2): 140-145.
[10]	ZHENG Guo-Tong , SU Ru-Keng . One η-Meson Exchange Potential of Nucleon-Nucleon at Finite Temperature. Chinese Physics C, 1992, 16(2): 131-136.
[11]	WANG En-Ke , LI Jia-Rong . The Equation of State and Phase Structure in A Model with Dynamical Spontaneous Symmetry Breaking at Finite Temperature and Density. Chinese Physics C, 1992, 16(4): 344-351.
[12]	ZHENG Guo-Tong , SU Ru-Keng . π AND σ MESON EXCHANGE POTENTIALS OF NUCLEON-NUCLEON INTERACTION AT FINITE TEMPERATURE. Chinese Physics C, 1990, 14(3): 220-227.
[13]	LOU Sen-Yue , NI Guang-Jiong . VARIATIONAL ANALYSIS OF THE GROSS-NEVEU MODEL AT ZERO AND FINITE TEMPERATURE. Chinese Physics C, 1990, 14(3): 228-235.
[14]	WANG En-Ke , LI Jia-Rong . CHIRAL PHASE TRANSITION IN A MODEL WITH DYNAMICAL SPONTANEOUS-SYMMETRY-BREAKING AT FINITE TEMPERATURE AND DENSITY. Chinese Physics C, 1990, 14(11): 980-990.
[15]	BI Pin-Zhen . KAONS CONDENSATION AT FINITE TEMPEATURE. Chinese Physics C, 1989, 13(3): 219-221.
[16]	WANG En-Ke , LI Jia-Rong . DECONFINEMENT TRANSITION OF NONTOPOLOGICAL SOLITON MODEL AT FINITE TEMPERATURE. Chinese Physics C, 1989, 13(11): 1003-1006.
[17]	CHEN Tao , SU Ru-Keng . THE ONE PION EXCHANGE POTENTIAL AT FINITE TEMPERATURE. Chinese Physics C, 1988, 12(1): 140-144.
[18]	WANG Qin-Mou . THERMODYNAMICAL PROPERTIES OF GAUGE THEORIES AT FINITE TEMPERATURE AND CHEMICAL POTENTIAL (Ⅱ). Chinese Physics C, 1987, 11(2): 182-185.
[19]	WANG Qin-Mou . THERMODYNAMICAL PROPERTIES OF GAUGE THEORIES AT FINITE TEMPERATURE AND CHEMICAL POTENTIAL. Chinese Physics C, 1986, 10(1): 24-31.
[20]	SU Ru-Keng , BI Pin-Zhen . THE ELEMENTARY EXCITATION SPECTRA OF MOHAPATRA-SENJANOVIC MODEL AT FINITE TEMPERATURE. Chinese Physics C, 1984, 8(2): 177-184.

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HUANG Jing-Yi, CAI Sheng-Shan, HU Si-Zhu and SU Ru-Keng. Chiral Bag Model at Finite Temperature[J]. Chinese Physics C, 1992, 16(6): 494-498.

HUANG Jing-Yi, CAI Sheng-Shan, HU Si-Zhu and SU Ru-Keng. Chiral Bag Model at Finite Temperature[J]. Chinese Physics C, 1992, 16(6): 494-498. shu

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Received: 1900-01-01
Revised: 1900-01-01

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1.
沈阳化工大学材料科学与工程学院沈阳 110142

Chiral Bag Model at Finite Temperature

Corresponding author: HUANG Jing-Yi,

Department of Physics,Fudan University,Shanghai 200433

Received Date: 1900-01-01
Accepted Date: 1900-01-01
Available Online: 1992-06-05

Abstract: By taking the thermodynamical contributions of the pion mesons cloud outside the bag into account,the chiral bag model is extended to finite temperature.The temperature dependence of the radius of the chiral bag and the critical temperature of quark deconfinement are given.