Tarasov theoretical and mathematical physics volume 41 pages 863 867 1979 cite this article.
E s egorian o v tarasov theor mat fiz 41 1979 26.
Zharkov the gell mann low function of qcd in the three loop approximation 1980 phys.
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41 1979 26 32 theor math phys.
41 1979 26 32 theor math phys.
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.
Egorian dubna jinr o v.
41 863 1979 teor.
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 429.
Larin e a randall laboratory of physics university of michigan ann arbor m148109 usa b nikhef p o.
Jones michigan u phys rev.
The result for the fl function coincides with the previous calculation o v.
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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.
Van ritbergen a j a m.
Two loop renormalization of the qcd in an arbitrary gauge.
The result for the β function coincides with the previous calculation o v.
Box 41882 1009 db amsterdam the netherlands institute for nuclear research of the russian academy of sciences.
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.
41 26 google scholar 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.
Vladimirov dubna jinr.
