E S Egorian O V Tarasov Theor Mat Fiz 41 1979 26

B 93 1980 429.

E s egorian o v tarasov theor mat fiz 41 1979 26.

Egorian dubna jinr o v. Larin in proceedings of the international school particles and cosmology baksan neutrino observatory of inr 1993 edited by e n. If the address matches an existing account you will receive an email with instructions to reset your password. Renormalization of quantum chromodynamics in the two loop approximation in an arbitrary gauge.

The calculation of the one loop fl function in quantum chromodynamics qcd has lead to the discovery of the asymptotic freedom in this model and to establishing qcd as the theory of strong. Box 41882 1009 db amsterdam the netherlands institute for nuclear research of the russian academy of sciences. Van ritbergen a j a m. 41 1979 26 32 theor math phys.

41 1979 26 32 theor math phys. Jones michigan u phys rev. Tarasov dubna jinr teor mat fiz. 41 1979 863 867 16 the two loop beta function for a g 1 x g 2 gauge theory.

Tarasov moscow state u a a. 41 863 1979 teor. Egorian dubna jinr o v. The recent qcd calculations of the five loop beta function and of r e e to o alpha s 4 provide one more term in the banks zaks expansion in 16 5 nf.

B 93 1980 4291. Vladimirov dubna jinr. 41 26 google scholar o v. Tarasov dubna jinr teor mat fiz.

A technique for calculating the gamma matrix structures of the diagrams of a total four fermion interaction with infinite number of vertices in d 2 epsilon dimensional regularization. Zharkov the gell mann low function of qcd in the three loop approximation 1980 phys. Elsevier physics letters b 400 1997 379 384 15 may 1997 physics letters b the four loop 3 function in quantum chromodynamics c t. Tarasov theoretical and mathematical physics volume 41 pages 863 867 1979 cite this article.

The result for the fl function coincides with the previous calculation o v.