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E s egorian o v tarasov theor mat fiz 41 1979 26.
Tarasov moscow state u a a.
Vladimirov dubna jinr.
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41 1979 26 32 theor math phys.
Tarasov theoretical and mathematical physics volume 41 pages 863 867 1979 cite this article.
Egorian dubna jinr o v.
Tarasov dubna jinr teor mat fiz.
Box 41882 1009 db amsterdam the netherlands institute for nuclear research of the russian academy of sciences.
The result for the β function coincides with the previous calculation o v.
Tarasov dubna jinr teor mat fiz.
41 26 google scholar o v.
Egorian dubna jinr o v.
Elsevier physics letters b 400 1997 379 384 15 may 1997 physics letters b the four loop 3 function in quantum chromodynamics c t.
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.
Two loop renormalization of the qcd in an arbitrary gauge.
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.
41 1979 863 867 16 the two loop beta function for a g 1 x g 2 gauge theory.
Renormalization of quantum chromodynamics in the two loop approximation in an arbitrary gauge.
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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 fl function coincides with the previous calculation o v.
Van ritbergen a j a m.