Abstract
We suggest how to consistently calculate the anomalous dimension γ∗ of the ψψ operator in finite order perturbation theory at an infrared fixed point for asymptotically free theories. If the n+1 loop beta function and n loop anomalous dimension are known, then γ∗ can be calculated exactly and fully scheme independently in a Banks-Zaks expansion through O(Δfn), where Δf=Nf-Nf, Nf is the number of flavors, and Nf is the number of flavors above which asymptotic freedom is lost. For a supersymmetric theory, the calculation preserves supersymmetry order by order in Δf. We then compute γ∗ through O(Δf2) for supersymmetric QCD in the dimensional reduction scheme and find that it matches the exact known result. We find that γ∗ is astonishingly well described in perturbation theory already at the few loops level throughout the entire conformal window. We finally compute γ∗ through O(Δf3) for QCD and a variety of other nonsupersymmetric fermionic gauge theories. Small values of γ∗ are observed for a large range of flavors.
Original language | English |
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Article number | 071601 |
Journal | Physical Review Letters |
Volume | 117 |
Issue number | 7 |
Pages (from-to) | 1-6 |
ISSN | 0031-9007 |
DOIs | |
Publication status | Published - 2016 |
Keywords
- hep-th
- hep-lat
- hep-ph