Full metadata record
| DC Field | Value | Language |
|---|---|---|
| dc.contributor.author | Yeh, TW | en_US |
| dc.date.accessioned | 2019-04-03T06:39:55Z | - |
| dc.date.available | 2019-04-03T06:39:55Z | - |
| dc.date.issued | 2002-05-01 | en_US |
| dc.identifier.issn | 2470-0010 | en_US |
| dc.identifier.uri | http://dx.doi.org/10.1103/PhysRevD.65.094019 | en_US |
| dc.identifier.uri | http://hdl.handle.net/11536/28829 | - |
| dc.description.abstract | The 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.language.iso | en_US | en_US |
| dc.title | eta-eta ' mixing and the next-to-leading-order power correction | en_US |
| dc.type | Article | en_US |
| dc.identifier.doi | 10.1103/PhysRevD.65.094019 | en_US |
| dc.identifier.journal | PHYSICAL REVIEW D | en_US |
| dc.citation.volume | 65 | en_US |
| dc.citation.issue | 9 | en_US |
| dc.citation.spage | 0 | en_US |
| dc.citation.epage | 0 | en_US |
| dc.contributor.department | 物理研究所 | zh_TW |
| dc.contributor.department | Institute of Physics | en_US |
| dc.identifier.wosnumber | WOS:000175914500056 | en_US |
| dc.citation.woscount | 6 | en_US |
| Appears in Collections: | Articles | |
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