数学物理学报(英文版) ›› 1988, Vol. 8 ›› Issue (2): 211-226.

• 论文 • 上一篇    下一篇

CALCULATION OF α3 COEFFICIENT OF SCALAR FIELD BY POINT SEPARATION METHOD

许殿彦   

  1. Center of Theoretical Physics, CCAST(World Laboratory) Beijing Dept. of Comp. Sci. & Tech., Peking University
  • 收稿日期:1987-04-03 出版日期:1988-06-25 发布日期:1988-06-25
  • 基金资助:
    Projects supported by the Science Fund of the Chinese Academy of Sciences.

CALCULATION OF α3 COEFFICIENT OF SCALAR FIELD BY POINT SEPARATION METHOD

Xu Dianyan   

  1. Center of Theoretical Physics, CCAST(World Laboratory) Beijing Dept. of Comp. Sci. & Tech., Peking University
  • Received:1987-04-03 Online:1988-06-25 Published:1988-06-25
  • Supported by:
    Projects supported by the Science Fund of the Chinese Academy of Sciences.

摘要: The α3 coefficient of scalar field in arbitrary Riemann space-time background is calculated by point separation method in this article. The primary expression of α3 involves 25 invariants. Using the identities derived in the appendix, we can reduce α3 from 25 invariants to 17 invariants which agree with Gilkey's formula for α3 coefficient of the scalar field derived by geometric methods and reasons. Recently we derived two important invariant identilies, using these identities we can reduce α3 from 17 invariants to 15 invariants which would much simplify the calculation of the energymomentum tensor of vacuum polarization.

Abstract: The α3 coefficient of scalar field in arbitrary Riemann space-time background is calculated by point separation method in this article. The primary expression of α3 involves 25 invariants. Using the identities derived in the appendix, we can reduce α3 from 25 invariants to 17 invariants which agree with Gilkey's formula for α3 coefficient of the scalar field derived by geometric methods and reasons. Recently we derived two important invariant identilies, using these identities we can reduce α3 from 17 invariants to 15 invariants which would much simplify the calculation of the energymomentum tensor of vacuum polarization.