2002/12/31 by S. S. Agaev, N. G. Stefanis · 1 citation
Physics and Astronomy · #Context (archaeology) #Coupling (piping) #Form factor (electronics) #Gluon #High-Energy Particle Collisions Research #Massless particle #Particle physics theoretical and experimental studies #Quantum Chromodynamics and Particle Interactions #Range (aeronautics) #Renormalon #hep-ph
paper · pdf · doi:10.1140/epjc/s2003-01463-2
published as Eur.Phys.J. C32 (2004) 507-528 · 38 pages, RevTeX4 used. 18 figures as PS/EPS files. Discussion extended; some typos corrected; change of renormalization scale to 1 GeV. Main results unchanged. Matches version to be published in Eur. Phys. J. C
arxiv created 2003/11/03 · openalex publication_date 2004/02/01 · arxiv updated 2009/11/30 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
Employing the standard hard-scattering approach (HSA) in conjunction with the running-coupling (RC) method, the latter joined with the infrared-renormalon calculus, we compute power-suppressed corrections ∼ 1/Q2n, n=1, 2,... to the massless η′ meson - virtual gluon transition form factor (FF) Q2Fη′g*g*(Q2,ω). Contributions to the form factor from the quark and gluon components of the η′ meson are taken into account. Analytic expressions for the FF's Fη′gg*(Q2,ω=± 1) and Fη′g*g*(Q2,ω=0) are also presented, as well as Borel transforms B[Q2Fη′g*g*](u) and resummed expressions. It is shown that except for ω=± 1, 0, the Borel transform contains an infinite number of infrared renormalon poles. It is demonstrated that in the explored range of the total gluon virtuality 1 \rm GeV2 ≤ Q2 ≤ 25 \rm GeV2, power corrections found with the RC method considerably enhance the FF Fη′g*g*(Q2, ω) relative to results obtained only in the context of the standard HSA with a ``frozen'' coupling.