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eta-eta ' mixing and the next-to-leading-order power correction

dc.citation.epage0en_US
dc.citation.issue9en_US
dc.citation.spage0en_US
dc.citation.volume65en_US
dc.citation.woscount6en_US
dc.contributor.authorYeh, TWen_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.date.accessioned2019-04-03T06:39:55Z
dc.date.available2019-04-03T06:39:55Z
dc.date.issued2002-05-01en_US
dc.description.abstractThe next-to-leading-order O(1/Q(4)) power corrections for etagamma and eta(')gamma form factors are evaluated and employed to explore the eta-eta(') mixing. The parameters of the two-mixing-angle scheme are extracted from the data for form factors, two-photon decay widths, and radiative J/psi decays. The chi(2) analysis gives the result f(eta1)=(1.16+/-0.06)f(pi),f(eta8)=(1.33+/-0.23)f(pi),theta(1)=-9degrees+/-3degrees,theta(8)=-21.3degrees+/-2.3degrees, where f(eta1(8)) and theta(1(8)) are the decay constants and the mixing angles for the singlet (octet) state. In addition, we arrive at a stringent range for f(eta)('c):-10 MeVless than or equal tof(eta)('c)less than or equal to-4 MeV.en_US
dc.identifier.doi10.1103/PhysRevD.65.094019en_US
dc.identifier.issn2470-0010en_US
dc.identifier.journalPHYSICAL REVIEW Den_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevD.65.094019en_US
dc.identifier.urihttps://ir.lib.nycu.edu.tw/handle/11536/28829
dc.identifier.wosnumberWOS:000175914500056en_US
dc.language.isoen_USen_US
dc.titleeta-eta ' mixing and the next-to-leading-order power correctionen_US
dc.typeArticleen_US

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