In quantum chromodynamics (and also N = 1 super quantum chromodynamics) with massless flavors, if the number of flavors, Nf, is sufficiently small (i.e. small enough to guarantee asymptotic freedom, depending on the number of colors), the theory can flow to an interacting conformal fixed point of the renormalization group.
[1] If the value of the coupling at that point is less than one (i.e. one can perform perturbation theory in weak coupling), then the fixed point is called a Banks–Zaks fixed point.
The existence of the fixed point was first reported in 1974 by Belavin and Migdal[2] and by Caswell,[3] and later used by Banks and Zaks [4] in their analysis of the phase structure of vector-like gauge theories with massless fermions.
More specifically, suppose that we find that the beta function of a theory up to two loops has the form where
are positive constants.
It follows that when the theory flows to the IR it is a conformal, weakly coupled theory with coupling
For the case of a non-Abelian gauge theory with gauge group
and Dirac fermions in the fundamental representation of the gauge group for the flavored particles we have where
is the number of colors and
the number of flavors.
in order for the Banks–Zaks fixed point to appear.
Note that this fixed point only occurs if, in addition to the previous requirement on
(which guarantees asymptotic freedom), where the lower bound comes from requiring
remains positive while
is still negative (see first equation in article) and one can solve
with real solutions for
was first correctly computed by Caswell,[3] while the earlier paper by Belavin and Migdal [2] has a wrong answer.
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