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dc.contributor.authorYeh, TWen_US
dc.date.accessioned2019-04-03T06:40:03Z-
dc.date.available2019-04-03T06:40:03Z-
dc.date.issued2002-04-01en_US
dc.identifier.issn2470-0010en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevD.65.074016en_US
dc.identifier.urihttp://hdl.handle.net/11536/28911-
dc.description.abstractAs is well recognized, the asymptotic of the perturbative QCD prediction for the pion form factor is much smaller than the upper end of the data. We investigate this problem. We first evaluate the next-to-leading-order (NLO) power correction for the pion form factor. The corrected form factor contains nonperturbative parameters which are determined from a chi(2) fit to the data. Interpreting these parameters leads to the fact that the involved strong interaction coupling constant should be identified as an effective coupling constant under a nonperturbative QCD vacuum. If the scale associated with the effective coupling constant is identified as <x>(2)Q(2), then Q(2), the momentum transfer square for the pion form factor to be measured, can have a value about 1 GeV2, and <x>, the averaged momentum fraction variable, can locate around 0.5. This circumstance is consistent with the asymptotic model for the pion wave function.en_US
dc.language.isoen_USen_US
dc.titleApplicability of perturbative QCD and NLO power corrections for the pion form factoren_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevD.65.074016en_US
dc.identifier.journalPHYSICAL REVIEW Den_US
dc.citation.volume65en_US
dc.citation.issue7en_US
dc.citation.spage0en_US
dc.citation.epage0en_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.identifier.wosnumberWOS:000174980100059en_US
dc.citation.woscount8en_US
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