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https://doi.org/10.1016/s0550-3213(96)00532-9
Copy DOIJournal: Nuclear Physics B | Publication Date: Dec 1, 1996 |
Citations: 26 |
We propose a renormalon-inspired resummation of QCD perturbation theory based on approximating the renormalization scheme (RS)-invariant effective charge beta-function coefficients by the portion containing the highest power of b= 1 6 (11N−2N f) for SU( N) QCD with N f quark flavours. This can be accomplished using exact large- N f all-orders results. The resulting resummation is RS invariant and the exact next-to-leading order (NLO) and next-to-NLO (NNLO) coefficients in any RS are included. This improves on a previously employed naive resummation of the leading- b piece of the perturbative coefficients which is RS dependent, making its comparison with fixed-order perturbative results ambiguous. The RS-invariant resummation is used to assess the reliability of fixed-order perturbation theory for the e + e − R-ratio, the analogous τ-lepton decay ratio R τ and deep inelastic scattering (DIS) sum rules, by comparing it with the exact NNLO results in the effective charge RS. For the R-ratio and R,, where large-order perturbative behaviour is dominated by a leading ultra-violet renormalon singularity, the comparison indicates fixed-order perturbation theory to be very reliable. For DIS sum rules, which have a leading infra-red renormalon singularity, the performance is rather poor. In this way we estimate that at LEP/ SLD energies ideal data on the R-ratio could determine α s ( M z ) to three-significant figures, and for the R τ we estimate a theoretical uncertainty δα s ( m τ ) ≅ 0.008 corresponding to δα s ( M z ) ≅ 0.001 This encouragingly small uncertainty is much less than has recently been deduced from comparison with the ambiguous naive resummation.
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