Abstract:
The Gell-Mann-Low function in QCD $\beta(g)(g=\bar g^2/16 \pi^2$,where $\bar g$ — is the coupling constant in the Lagrangian) is shown to behave in the strong-coupling region as $\beta_\infty g^\alpha$, where $\alpha\approx -13 $ and $\beta_\infty \sim 10^5$.