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

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

Larin e a randall laboratory of physics university of michigan ann arbor m148109 usa b nikhef p o. B 93 1980 4291. 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. The result for the β function coincides with the previous calculation o v.

Egorian dubna jinr o v. 41 1979 26 32 theor math phys. Renormalization of quantum chromodynamics in the two loop approximation in an arbitrary gauge. Tarasov dubna jinr teor mat fiz.

The result for the fl function coincides with the previous calculation o v. 41 26 google scholar o v. Tarasov theoretical and mathematical physics volume 41 pages 863 867 1979 cite this article. 41 1979 26 32 theor math phys.

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. Elsevier physics letters b 400 1997 379 384 15 may 1997 physics letters b the four loop 3 function in quantum chromodynamics c t. 41 863 1979 teor.

Zharkov the gell mann low function of qcd in the three loop approximation 1980 phys. 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. 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.

Vladimirov dubna jinr. Van ritbergen a j a m. Jones michigan u phys rev. Tarasov moscow state u a a.

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.