The Generalized Scheme-Independent Crewther Relation in QCD
arXiv:1611.07249 · doi:10.1016/j.physletb.2017.05.022
Abstract
The Principle of Maximal Conformality (PMC) provides a systematic way to set the renormalization scales order-by-order for any perturbative QCD process. The resulting predictions are independent of the choice of renormalization scheme, a requirement of renormalization group invariance. The Crewther relation, which was originally derived for conformal theory, provides a remarkable connection between two observables when the function vanishes. The "Generalized Crewther Relation" relates these two observables for physical QCD with nonzero function; specifically, it connects the non-singlet Adler function () to the Bjorken sum rule coefficient for polarized deep-inelastic electron scattering () at leading twist. A scheme-dependent -term appears in the analysis in order to compensate for the conformal symmetry breaking (CSB) terms from perturbative QCD. In conventional analyses, this normally leads to unphysical dependence in both the choice of the renormalization scheme and the choice of the initial scale at any finite order. However, by applying PMC scale-setting, we can fix the scales of the QCD coupling unambiguously at every order of pQCD. ...... Thus one obtains a new generalized Crewther relation for QCD which connects two effective charges, , at their respective physical scales. This identity is independent of the choice of the renormalization scheme at any finite order, and the dependence on the choice of the initial scale is negligible. Similar scale-fixed commensurate scale relations also connect other physical observables at their physical momentum scales, thus providing convention-independent, fundamental precision tests of QCD.
7 pages, 3 figures. Revised version accepted by Phys.Lett.B
References in corpus (5)
- Adler Function, Bjorken Sum Rule, and the Crewther Relation to Order alpha_s^4 in a General Gauge Theory
- Self-Consistency Requirements of the Renormalization Group for Setting the Renormalization Scale
- Degeneracy Relations in QCD and the Equivalence of Two Systematic All-Orders Methods for Setting the Renormalization Scale
- Implications of the Principle of Maximum Conformality for the QCD Strong Coupling
- Setting the Renormalization Scale in pQCD: Comparisons of the Principle of Maximum Conformality with the Sequential Extended Brodsky-Lepage-Mackenzie Approach
Cited by in corpus (15)
- The QCD Renormalization Group Equation and the Elimination of Fixed-Order Scheme-and-Scale Ambiguities Using the Principle of Maximum Conformality
- QCD Running Couplings and Effective Charges
- A novel demonstration of the renormalization group invariance of the fixed-order predictions using the principle of maximum conformality and the -scheme coupling
- Implications of the Principle of Maximum Conformality for the QCD Strong Coupling
- Extending the Predictive Power of Perturbative QCD
- Renormalization scheme and gauge (in)dependence of the generalized Crewther relation: what are the real grounds of the -factorization property?
- Determination of the top-quark running mass via its perturbative relation to the on-shell mass with the help of principle of maximum conformality
- Properties of the decay using the approximate -corrections and the principle of maximum conformality
- Generalized Crewther relation and a novel demonstration of the scheme independence of commensurate scale relations up to all orders
- pQCD running couplings finite and monotonic in the infrared: when do they reflect the holomorphic properties of spacelike observables?
- New determination of using the three-loop QCD corrections for the semi-leptonic decays
- Riemann function contributions to terms of Adler D-function and Bjorken polarized sum rule in QCD: results and consequences
- The Principle of Maximum Conformality Correctly Resolves the Renormalization-Scheme-Dependence Problem
- Scale-invariant total decay width using the novel method of characteristic operator
- Updated Determination of Ellis-Jaffe Sum Rules up to QCD corrections