The structure of generic anomalous dimensions and no-π theorem for massless propagators

Abstract Extending an argument of [1] for the case of 5-loop massless propagators we prove a host of new exact model-independent relations between contributions proportional to odd and even zetas in generic MS¯ $$ \overline{\mathrm{MS}} $$ anomalous dimensions as well as in generic massless correlat...

Full description

Bibliographic Details
Main Authors: P. A. Baikov, K. G. Chetyrkin
Format: Article
Language:English
Published: SpringerOpen 2018-06-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP06(2018)141
id doaj-a7ce89aa24154d259cdeec1c7421f85f
record_format Article
spelling doaj-a7ce89aa24154d259cdeec1c7421f85f2020-11-25T02:01:47ZengSpringerOpenJournal of High Energy Physics1029-84792018-06-012018612510.1007/JHEP06(2018)141The structure of generic anomalous dimensions and no-π theorem for massless propagatorsP. A. Baikov0K. G. Chetyrkin1Skobeltsyn Institute of Nuclear Physics, Lomonosov Moscow State UniversityII Institut für Theoretische Physik, Universität HamburgAbstract Extending an argument of [1] for the case of 5-loop massless propagators we prove a host of new exact model-independent relations between contributions proportional to odd and even zetas in generic MS¯ $$ \overline{\mathrm{MS}} $$ anomalous dimensions as well as in generic massless correlators. In particular, we find a new remarkable connection between coefficients in front of ζ 3 and ζ 4 in the 4-loop and 5-loop contributions to the QCD β-function respectively. It leads to a natural explanation of a simple mechanics behind mysterious cancellations of the π-dependent terms in one-scale Renormalization Group (RG) invariant Euclidean quantities recently discovered in [2]. We give a proof of this no-π theorem for a general case of (not necessarily scheme-independent) one-scale massless correlators. All π-dependent terms in the six-loop coefficient of an anomalous dimension (or a β-function) are shown to be explicitly expressible in terms of lower order coefficients for a general one-charge theory. For the case of a scalar O(n) ϕ 4 theory all our predictions for π-dependent terms in 6-loop anomalous dimensions are in full agreement with recent results of [3–5].http://link.springer.com/article/10.1007/JHEP06(2018)141Perturbative QCDRenormalization Group
collection DOAJ
language English
format Article
sources DOAJ
author P. A. Baikov
K. G. Chetyrkin
spellingShingle P. A. Baikov
K. G. Chetyrkin
The structure of generic anomalous dimensions and no-π theorem for massless propagators
Journal of High Energy Physics
Perturbative QCD
Renormalization Group
author_facet P. A. Baikov
K. G. Chetyrkin
author_sort P. A. Baikov
title The structure of generic anomalous dimensions and no-π theorem for massless propagators
title_short The structure of generic anomalous dimensions and no-π theorem for massless propagators
title_full The structure of generic anomalous dimensions and no-π theorem for massless propagators
title_fullStr The structure of generic anomalous dimensions and no-π theorem for massless propagators
title_full_unstemmed The structure of generic anomalous dimensions and no-π theorem for massless propagators
title_sort structure of generic anomalous dimensions and no-π theorem for massless propagators
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2018-06-01
description Abstract Extending an argument of [1] for the case of 5-loop massless propagators we prove a host of new exact model-independent relations between contributions proportional to odd and even zetas in generic MS¯ $$ \overline{\mathrm{MS}} $$ anomalous dimensions as well as in generic massless correlators. In particular, we find a new remarkable connection between coefficients in front of ζ 3 and ζ 4 in the 4-loop and 5-loop contributions to the QCD β-function respectively. It leads to a natural explanation of a simple mechanics behind mysterious cancellations of the π-dependent terms in one-scale Renormalization Group (RG) invariant Euclidean quantities recently discovered in [2]. We give a proof of this no-π theorem for a general case of (not necessarily scheme-independent) one-scale massless correlators. All π-dependent terms in the six-loop coefficient of an anomalous dimension (or a β-function) are shown to be explicitly expressible in terms of lower order coefficients for a general one-charge theory. For the case of a scalar O(n) ϕ 4 theory all our predictions for π-dependent terms in 6-loop anomalous dimensions are in full agreement with recent results of [3–5].
topic Perturbative QCD
Renormalization Group
url http://link.springer.com/article/10.1007/JHEP06(2018)141
work_keys_str_mv AT pabaikov thestructureofgenericanomalousdimensionsandnoptheoremformasslesspropagators
AT kgchetyrkin thestructureofgenericanomalousdimensionsandnoptheoremformasslesspropagators
AT pabaikov structureofgenericanomalousdimensionsandnoptheoremformasslesspropagators
AT kgchetyrkin structureofgenericanomalousdimensionsandnoptheoremformasslesspropagators
_version_ 1724955809453965312