EPJ Web Conf.
Volume 137, 2017XIIth Quark Confinement and the Hadron Spectrum
|Number of page(s)||10|
|Section||Section E: QCD and New Physics|
|Published online||22 March 2017|
Probing QCD perturbation theory at high energies with continuum extrapolated lattice data
School of Mathematics & Hamilton Mathematics Institute, Trinity College Dublin, Dublin 2, Ireland
a e-mail: firstname.lastname@example.org
Published online: 22 March 2017
Precision tests of QCD perturbation theory are not readily available from experimental data. The main reasons are systematic uncertainties due to the confinement of quarks and gluons, as well as kinematical constraints which limit the accessible energy scales. We here show how continuum extrapolated lattice data may overcome such problems and provide excellent probes of renormalized perturbation theory. This work corresponds to an essential step in the ALPHA collaboration’s project to determine the Λ-parameter in 3-flavour QCD. I explain the basic techniques used in the high energy regime, namely the use of mass-independent renormalization schemes for the QCD coupling constant in a finite Euclidean space time volume. When combined with finite size techniques this allows one to iteratively step up the energy scale by factors of 2, thereby quickly covering two orders of magnitude in scale. We may then compare perturbation theory (with β-functions available up to 3-loop order) to our non-perturbative data for a 1-parameter family of running couplings. We conclude that a target precision of 3 percent for the Λ-parameter requires non-perturbative data up to scales where αs ≈ 0.1, whereas the apparent precision obtained from applying perturbation theory around αs ≈ 0.2 can be misleading. This should be taken as a general warning to practitioners of QCD perturbation theory.
© The Authors, published by EDP Sciences, 2017
This is an Open Access article distributed under the terms of the Creative Commons Attribution License 4.0, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
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