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

Renormalization of quantum chromodynamics in the two loop approximation in an arbitrary gauge.

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

Vladimirov dubna jinr. The result for the β function coincides with the previous calculation o v. The result for the fl function coincides with the previous calculation o v. B 93 1980 4291.

Box 41882 1009 db amsterdam the netherlands institute for nuclear research of the russian academy of sciences. 41 863 1979 teor. Tarasov dubna jinr teor mat fiz. Two loop renormalization of the qcd in an arbitrary gauge.

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. Larin e a randall laboratory of physics university of michigan ann arbor m148109 usa b nikhef p o. If the address matches an existing account you will receive an email with instructions to reset your password. Zharkov the gell mann low function of qcd in the three loop approximation 1980 phys.

Jones michigan u phys rev. Egorian dubna jinr o v. Van ritbergen a j a m. Elsevier physics letters b 400 1997 379 384 15 may 1997 physics letters b the four loop 3 function in quantum chromodynamics c t.

Larin in proceedings of the international school particles and cosmology baksan neutrino observatory of inr 1993 edited by e n. 41 1979 26 32 theor math phys. B 93 1980 429. Tarasov moscow state u a a.

Tarasov dubna jinr teor mat fiz. 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. Tarasov theoretical and mathematical physics volume 41 pages 863 867 1979 cite this article. 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.