paper

Operator mixing in massless QCD-like theories and Poincare'-Dulac theorem

arXiv:2103.16220 · doi:10.1140/epjc/s10052-022-10551-2

Abstract

Recently, a geometric approach to operator mixing in massless QCD-like theories -- that involves canonical forms based on the Poincare'-Dulac theorem for the linear system that defines the renormalized mixing matrix in the coordinate representation -- has been advocated in arXiv:2103.15527 . As a consequence, a classification of operator mixing in four cases -- depending on the canonical forms of , with the matrix of the anomalous dimensions and the beta function -- has been proposed: (I) nonresonant diagonalizable, (II) resonant diagonalizable, (III) nonresonant nondiagonalizable, (IV) resonant nondiagonalizable. In particular, in arXiv:2103.15527 a detailed analysis of the case (I) -- where operator mixing reduces to all orders of perturbation theory to the multiplicatively renormalizable case -- has been provided. In the present paper, following the aforementioned approach, we work out in the remaining three cases the canonical forms for to all orders of perturbation theory, the corresponding UV asymptotics of , and the physics interpretation. We also work out in detail physical realizations of the cases (I) and (II).

35 pages, formulas unchanged, but some comments on the UV asymptotics corrected, physical realizations of the resonant case and new references added

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