Exploring arbitrarily high orders of optimized perturbation theory in QCD with nf→1612

Perturbative QCD with nf flavours of massless quarks becomes simple in the hypothetical limit nf→1612, where the leading β-function coefficient vanishes. The Banks–Zaks (BZ) expansion in a0≡8321(1612−nf) is straightforward to obtain from perturbative results in MS‾ or any renormalization scheme (RS)...

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Main Author: P.M. Stevenson
Format: Article
Language:English
Published: Elsevier 2016-09-01
Series:Nuclear Physics B
Online Access:http://www.sciencedirect.com/science/article/pii/S0550321316302000
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author P.M. Stevenson
author_facet P.M. Stevenson
author_sort P.M. Stevenson
collection DOAJ
description Perturbative QCD with nf flavours of massless quarks becomes simple in the hypothetical limit nf→1612, where the leading β-function coefficient vanishes. The Banks–Zaks (BZ) expansion in a0≡8321(1612−nf) is straightforward to obtain from perturbative results in MS‾ or any renormalization scheme (RS) whose nf dependence is ‘regular’. However, ‘irregular’ RS's are perfectly permissible and should ultimately lead to the same BZ results. We show here that the ‘optimal’ RS determined by the Principle of Minimal Sensitivity does yield the same BZ-expansion results when all orders of perturbation theory are taken into account. The BZ limit provides an arena for exploring optimized perturbation theory at arbitrarily high orders. These explorations are facilitated by a ‘master equation’ expressing the optimization conditions in the fixed-point limit. We find an intriguing strong/weak coupling duality a→a⁎2/a about the fixed point a⁎.
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spelling doaj.art-39755823cd1d49f988639a3a90bbb9f02022-12-22T02:17:52ZengElsevierNuclear Physics B0550-32131873-15622016-09-01910C46949510.1016/j.nuclphysb.2016.07.017Exploring arbitrarily high orders of optimized perturbation theory in QCD with nf→1612P.M. StevensonPerturbative QCD with nf flavours of massless quarks becomes simple in the hypothetical limit nf→1612, where the leading β-function coefficient vanishes. The Banks–Zaks (BZ) expansion in a0≡8321(1612−nf) is straightforward to obtain from perturbative results in MS‾ or any renormalization scheme (RS) whose nf dependence is ‘regular’. However, ‘irregular’ RS's are perfectly permissible and should ultimately lead to the same BZ results. We show here that the ‘optimal’ RS determined by the Principle of Minimal Sensitivity does yield the same BZ-expansion results when all orders of perturbation theory are taken into account. The BZ limit provides an arena for exploring optimized perturbation theory at arbitrarily high orders. These explorations are facilitated by a ‘master equation’ expressing the optimization conditions in the fixed-point limit. We find an intriguing strong/weak coupling duality a→a⁎2/a about the fixed point a⁎.http://www.sciencedirect.com/science/article/pii/S0550321316302000
spellingShingle P.M. Stevenson
Exploring arbitrarily high orders of optimized perturbation theory in QCD with nf→1612
Nuclear Physics B
title Exploring arbitrarily high orders of optimized perturbation theory in QCD with nf→1612
title_full Exploring arbitrarily high orders of optimized perturbation theory in QCD with nf→1612
title_fullStr Exploring arbitrarily high orders of optimized perturbation theory in QCD with nf→1612
title_full_unstemmed Exploring arbitrarily high orders of optimized perturbation theory in QCD with nf→1612
title_short Exploring arbitrarily high orders of optimized perturbation theory in QCD with nf→1612
title_sort exploring arbitrarily high orders of optimized perturbation theory in qcd with nf 1612
url http://www.sciencedirect.com/science/article/pii/S0550321316302000
work_keys_str_mv AT pmstevenson exploringarbitrarilyhighordersofoptimizedperturbationtheoryinqcdwithnf1612