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《中国物理C》(英文)编辑部
2024年10月30日

Medium Effects and Thermal Instability in φ63 Theory

  • We calculate the effective mass and damping rate in φ63 theory at finite temperature by evaluating the real and imaginary parts of the one-loop self energies at the hard thermal loop (HTL) approximation. We show that there is thermal instability above a critical temperature Tc. The effective mass and damping rate are proportional to gT and gT respectively. We compare our results with those in hot QCD.
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  • [1] . Kapusta J I. Finite Temperature Field Theory, Cambridge University Press,1989,35—67 2. Bellac M Le. Thermal Finite Theory, Cambridge University Press,1996,150—188 3. Pisarski R D. Phys. Rev. Lett.,1989,63:1129;Braaten E, Pisarski R D. Nucl. Phys.,1990,B337:569 4. Thoma M H. New Development and Applications of Thermal Field Theory, hep-Ph/000101645. HOU De-Fu et al. Phys. Rev.1996,D54:7634 6. Collins J C. Renormalization, Cambridge University Press,1983,132—147 7. HOU De-Fu et al. European J. Phys.,1998,C4:129 8. GAO Song et al. Phys. Rev.,1994,C49:40 9. ZHANG Ben-Wei et al. Phys. Rev.,2000,C61:051302(R)10. Altherr T et al. Phys. Lett.,1991,B271:183
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Get Citation
XIONG Chun and HOU De-Fu. Medium Effects and Thermal Instability in φ63 Theory[J]. Chinese Physics C, 2002, 26(8): 753-758.
XIONG Chun and HOU De-Fu. Medium Effects and Thermal Instability in φ63 Theory[J]. Chinese Physics C, 2002, 26(8): 753-758. shu
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Received: 2002-02-06
Revised: 1900-01-01
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Medium Effects and Thermal Instability in φ63 Theory

    Corresponding author: XIONG Chun,
  • Institute of Particle Physics,Central China Normal University,Wuhan 430079,China

Abstract: We calculate the effective mass and damping rate in φ63 theory at finite temperature by evaluating the real and imaginary parts of the one-loop self energies at the hard thermal loop (HTL) approximation. We show that there is thermal instability above a critical temperature Tc. The effective mass and damping rate are proportional to gT and gT respectively. We compare our results with those in hot QCD.

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