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

41 863 1979 teor.

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

Tarasov moscow state u a a. 41 1979 26 32 theor math phys. Egorian dubna jinr o v. Van ritbergen a j a m.

Larin e a randall laboratory of physics university of michigan ann arbor m148109 usa b nikhef p o. The result for the β function coincides with the previous calculation o v. 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. Jones michigan u phys rev.

Tarasov theoretical and mathematical physics volume 41 pages 863 867 1979 cite this article. If the address matches an existing account you will receive an email with instructions to reset your password. Box 41882 1009 db amsterdam the netherlands institute for nuclear research of the russian academy of sciences. The result for the fl function coincides with the previous calculation o v.

Vladimirov dubna jinr. Zharkov the gell mann low function of qcd in the three loop approximation 1980 phys. Tarasov dubna jinr teor mat fiz. 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. 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. Renormalization of quantum chromodynamics in the two loop approximation in an arbitrary gauge.

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

B 93 1980 429.