Mixed quark-gluon condensate from instantons

Abstract

We calculate the vacuum expectation value of the dimension-5 "mixed" quark-gluon operator, $O_σ= \barψ(λ^a /2) σ_{μν} ψF_{μν}^a$, in the instanton vacuum. Within the $1/N_c$--expansion the QCD operator is replaced by an effective many-fermion operator, which is averaged over the effective theory of massive quarks derived from instantons. We find $m_0^2 \equiv \langle O_σ\rangle / \langle \barψψ\rangle \approx 4 \barρ^{-2} = 1.4 GeV^2$, somewhat larger than the estimate from QCD sum rules for the nucleon.