I've heard about people talking about the 1/N expansion as a mothod of nonperturbative QCD. This seems strange. In the 1/N expansion all you have is Feynman diagrams, which are by definition perturbative. Just resumming them to infinite orders doesn't really count as nonperturbative physics. Is it really jusified to think resummation has anything to do with noperturbative physics? Is there some subtle connection betweeen the two that I missed?
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1) On one hand, perturbative QCD means an expansion in the Yang-Mills coupling constant $g_{YM}$ for a fixed number of colors $N_c$. 2) On the other hand, the $1/N_c$ expansion means an expansion in $1/N_c$ for fixed 't Hooft coupling constant $$\lambda~:=~g^2_{YM}N_c.$$ (Here it is implicitly assumed that all dependence of $g_{YM}$ have been replaced, so that there are only dependences of $\lambda$ and $N_c$.) 3) The two expansions (1) and (2) are different. There are perturbative terms in the latter expansion that correspond to non-perturbative terms from the former point of view. 4) To convey the idea without going into the complications of actual QCD, consider for simplicity the function $$f~=~\exp\left[-\frac{1}{\lambda}\right]~=~\exp\left[-\frac{1}{g^2_{YM}N_c}\right].$$ On one hand, the expansion (1) of $f$ yields an expansion that is zero to all orders perturbatively in $g_{YM}$. On the other hand, the expansion (2) of $f$ is exact already after the zeroth-order term in $1/N_c$. |
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