Pion Wave Function from QCD Sum Rules with Nonlocal Condensates

dc.creatorRadyushkin, Anatoly
dc.date1994-06-06
dc.date.accessioned2026-07-07T03:56:54Z
dc.date.available2026-07-07T03:56:54Z
dc.descriptionWe investigate a model QCD sum rule for the pion wave function $φ_π(x)$ based on the non-diagonal correlator whose perturbative spectral density vanishes and $Φ(x,M^2)$, the theoretical side of the sum rule, consists of condensate contributions only. We study the dependence of $Φ(x,M^2)$ on the Borel parameter $M^2$ and observe that $Φ(x,M^2)$ has a humpy form, with the humps becoming more and more pronounced when $M^2$ increases. We demonstrate that this phenomenon reflects just the oscillatory nature of the higher states wave functions, while the lowest state wave function $φ_π(x)$ extracted from our QCD sum rule analysis,has no humps, is rather narrow and its shape is close to the asymptotic form $φ_π^{as}(x) = 6x(1-x)$.
dc.descriptionTalk at the Workshop "Continuous Advances in QCD", 11 pages + appended uuencoded ps file with 8 figures, Latex, CEBAF-TH-94-13
dc.identifierhttps://arxiv.org/abs/hep-ph/9406237
dc.identifierhttp://arxiv.org/abs/hep-ph/9406237
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/45180
dc.subjectHigh Energy Physics - Phenomenology
dc.titlePion Wave Function from QCD Sum Rules with Nonlocal Condensates
dc.typetext

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