dc.contributor.author | Kolcu, Onur Buğra | en_US |
dc.contributor.other | BESIII Collaboration | |
dc.date.accessioned | 2019-07-01T08:12:51Z | |
dc.date.available | 2019-07-01T08:12:51Z | |
dc.date.issued | 2017 | en_US |
dc.identifier.citation | Ablikim, M., Achasov, M. N., Ahmed, S., Albrecht, M., Amoroso, A., An, F. F., . . . Collaboration, B. (2017). Improved measurements of two-photon widths of the chi(cJ) states and helicity analysis for chi(c2) -> gamma gamma. Physical Review D, 96(9), 11. doi:10.1103/PhysRevD.96.092007 | en_US |
dc.identifier.issn | 2470-0010 | |
dc.identifier.issn | 2470-0029 | |
dc.identifier.uri | https://hdl.handle.net/20.500.12294/1524 | |
dc.description | Kolcu, Onur Buğra (Arel Author) | en_US |
dc.description.abstract | Based on 448.1 x 10(6) Psi(3686) events collected with the BESIII detector, the decays Psi(3686) -> gamma chi(cJ), chi(cJ) -> gamma gamma(J = 0, 1, 2) are studied. The decay branching fractions of chi(c0,2) -> gamma gamma are measured to be B(chi(c0) -> gamma gamma) = (1.93 +/- 0.08 +/- 0.05 +/- 0.05) x 10(-4) and B(chi(c2) -> gamma gamma) = (3.10 +/- 0.09 +/- 0.07 +/- 0.11) x 10(-4) which correspond to two-photon decay widths of Gamma(gamma gamma)(chi(c0)) = 2.03 +/- 0.08 +/- 0.06 +/- 0.13 keV and Gamma(gamma gamma)(chi(c2)) = 0.60 +/- 0.02 +/- 0.01 +/- 0.04 keV with a ratio of R = Gamma(gamma gamma)(chi(c2))/Gamma(gamma gamma)(chi(c0)) = 0.295 +/- 0.014 +/- 0.007 +/- 0.027, where the uncertainties are statistical, systematic and associated with the uncertainties of B(Psi(3686) -> gamma chi(c0,2)) and the total widths Gamma(chi(c0,2)), respectively. For the forbidden decay of chi(c1) -> gamma gamma, no signal is observed, and an upper limit on the two-photon width is obtained to be Gamma(gamma gamma)(chi(c1)) < 5.3 eV at the 90% confidence level. The ratio of the two-photon widths between helicity-zero and helicity-two components in the decay chi(c2) -> gamma gamma is also measured to be f(0/2) = Gamma(lambda=0)(gamma gamma) (chi(c2))/Gamma(lambda=2)(gamma gamma) (chi(c2)) = (0.0 +/- 0.6 +/- 1.2) x 10(-2), where the uncertainties are statistical and systematic, respectively. | en_US |
dc.language.iso | eng | en_US |
dc.publisher | Amer Physical Soc. | en_US |
dc.relation.ispartof | Physical Review D. | en_US |
dc.identifier.doi | 10.1103/PhysRevD.96.092007 | en_US |
dc.identifier.doi | 10.1103/PhysRevD.96.092007 | |
dc.rights | info:eu-repo/semantics/openAccess | en_US |
dc.title | Improved measurements of two-photon widths of the chi(cJ) states and helicity analysis for chi(c2) -> gamma gamma | en_US |
dc.type | article | en_US |
dc.department | Meslek Yüksekokulu, Optisyenlik Programı | en_US |
dc.authorid | https://orcid.org/0000-0002-9177-1286 | en_US |
dc.identifier.volume | 96 | en_US |
dc.identifier.issue | 9 | en_US |
dc.identifier.startpage | 1 | en_US |
dc.identifier.endpage | 11 | en_US |
dc.relation.publicationcategory | Makale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı | en_US |
dc.institutionauthor | Kolcu, Onur Buğra | en_US |